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MeJennifer said:The question is: can we have a coordinate system of space-time where all geodesics can be represented as straight lines.
To determine if a geodesic is straight that passes a warped region in space-time we would need a description of the curvature.
That's if why we cannot conclude that if dx/dt, dy/dt and dz/dt remains constant we have a straight line. Or in other words without a metric describing the warping at all places on the wordline we would not be able to conclude that.
This is exactly right. I have bolded the key statement. And in (pseudo-)Riemannian geometry we have a metric tensor from which, in this case, we can derive a connection, a mathematical expression in the partial derivatives of the metric tensor, from which we get a covariant derivative which finally gives us a Riemannian or Curvature tensor, which describes the curvature. All of these derivations are straight computations from the metric; that is a feature of Riemannian geometry. Once we have this mathematical machinery that determines the curvature, we can do further mathematical derivations to find the form of the geodesic equations.
Now if the Riemann tensor is not identically zero then the form of the geodesic equations is not linear. Translation into English; if spacetime has nonzero curvature somewhere, then the geodesics there cannot be straight lines. This again is a straight computation and so it really only depends on the metric. In a Riemannian geometry the metric determines the curvature, and the geodesics for non zero curvature are not linear